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JPH025250B2 - - Google Patents
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JPH025250B2 - - Google Patents

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Publication number
JPH025250B2
JPH025250B2 JP5218383A JP5218383A JPH025250B2 JP H025250 B2 JPH025250 B2 JP H025250B2 JP 5218383 A JP5218383 A JP 5218383A JP 5218383 A JP5218383 A JP 5218383A JP H025250 B2 JPH025250 B2 JP H025250B2
Authority
JP
Japan
Prior art keywords
fluid
laser
power
laser beam
temperature
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP5218383A
Other languages
Japanese (ja)
Other versions
JPS59176631A (en
Inventor
Futoshi Uchama
Susumu Shiratori
Mitsuo Kasamatsu
Koichi Tsukamoto
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP5218383A priority Critical patent/JPS59176631A/en
Publication of JPS59176631A publication Critical patent/JPS59176631A/en
Publication of JPH025250B2 publication Critical patent/JPH025250B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01JMEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
    • G01J5/00Radiation pyrometry, e.g. infrared or optical thermometry
    • G01J5/38Radiation pyrometry, e.g. infrared or optical thermometry using extension or expansion of solids or fluids

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Photometry And Measurement Of Optical Pulse Characteristics (AREA)

Description

【発明の詳細な説明】 この発明は、レーザ電力の測定方法に関し、特
に流体をレーザ光吸収負荷体として用いるレーザ
電力測定方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for measuring laser power, and more particularly to a method for measuring laser power using a fluid as a laser light absorbing load.

レーザ技術が生産加工機等に応用されるように
なるにつれて、レーザ光の出力が飛躍的に高出力
となつてきており、レーザ光の電力の測定がます
ます重要になつてきている。
As laser technology has come to be applied to production processing machines and the like, the output of laser light has become dramatically higher, and measurement of the power of laser light has become increasingly important.

従来、固体負荷体を用いてその温度変化からレ
ーザ光の電力を測定するレーザ電力測定法はある
が、上記のような高出力のレーザ光の電力測定は
材料の耐熱性、耐久性、信頼性などの点から困難
な面があり、高出力のレーザ光の電力測定方法と
しては十分なものはいまだ開発されていない。
Conventionally, there is a laser power measurement method that measures the power of laser light from temperature changes using a solid load, but the power measurement of high-output laser light as described above depends on the heat resistance, durability, and reliability of the material. There are many difficulties, and no method has yet been developed that is sufficient to measure the power of high-power laser light.

この発明は、上述の点にかんがみてなされたも
ので、流体をレーザ光吸収負荷体として用い、こ
の流体負荷体にレーザ光を入射させてレーザ光の
エネルギーを流体負荷体に直接吸収させると共
に、潜熱を潜熱回収装置によつて流体に回収さ
せ、この流体の温度変化と流体の流量からレーザ
光の電力を測定するレーザ電力測定方法を提供す
ることを目的とする。
The present invention has been made in view of the above points, and uses a fluid as a laser beam absorbing load, and allows the laser beam to be incident on the fluid load so that the energy of the laser beam is directly absorbed by the fluid load. It is an object of the present invention to provide a laser power measurement method that recovers latent heat into a fluid using a latent heat recovery device and measures the power of a laser beam from the temperature change of the fluid and the flow rate of the fluid.

この発明の原理は、炭酸ガスレーザのレーザ光
が水に良く吸収される性質を有していることを利
用して、簡単にレーザ電力を測定するものであ
る。すなわち、レーザ光を水に入射させること、
そのエネルギーは水に吸収されて、一部は水の温
度を上昇させるエネルギーとなり、他の一部は水
を蒸発させ水蒸気を発生させる潜熱のエネルギー
となる。そしてレーザ光のエネルギーが大きく大
電力となるにつれて、潜熱の発生も大きくなり、
水温の上昇測定のみでは入射したレーザ光の電力
を精度良く測定することができなくなる。この点
を補い電力を精度良く測定するために潜熱のエネ
ルギーを潜熱回収装置で水の温度上昇として回収
する。エネルギーによる水の温度上昇と流量との
2つを測定することによりレーザ光のレーザ電力
を測定することができる。以下図を用いてこの発
明を説明する。
The principle of this invention is to easily measure laser power by utilizing the property that the laser light of a carbon dioxide gas laser is well absorbed by water. That is, making laser light incident on water,
Some of this energy is absorbed by the water, and some of it becomes energy that increases the temperature of the water, and some of it becomes latent heat energy that evaporates the water and generates water vapor. As the energy of the laser beam increases and the power increases, the generation of latent heat also increases.
Measuring the rise in water temperature alone makes it impossible to accurately measure the power of the incident laser beam. In order to compensate for this point and measure electric power with high precision, latent heat energy is recovered as a rise in water temperature using a latent heat recovery device. The laser power of the laser beam can be measured by measuring the temperature rise of water due to energy and the flow rate. This invention will be explained below using the figures.

第1図はこの発明の一実施例をなすレーザ電力
計の構造を示す立体透視図である。同図におい
て、1は円筒状をした電力計本体であり、この電
力計本体1には流体Hを導入する導入パイプ2と
流体Hを排出する排出パイプ3が設けられてい
る。4は前記流体Hの流量を測定する流量計であ
り、導入パイプ2に設けられている。5,6は前
記流体Hの温度を測定するための温度センサであ
り、温度センサ5は流体負荷体にレーザ光を照象
する前の温度を測定するため導入パイプ2に設け
られ、温度センサ6は流体負荷体にレーザ光を照
射した後の流体速度を測定するために排出パイプ
3に設けられる。7は前記電力計本体1に導いた
流体Hをシヤワー式に散落下させるためのじよう
ろ、8は円錐状の多層メツシユ、9は前記流体H
を照射位置に導く流体負荷体整形板で、陣笠状の
本体9Aとその上に間隔を置いて設けられた同じ
く陣笠状の副体9Bとからなり、本体9Aは中央
上部に孔があけられており、この孔をおおうよう
に副体9Bが設けられている。また、本体9Aは
電力計本体1の内面との間に部分的に間隙10を
形成しており、その他は密閉するようになつてい
る。11は前記流体負荷体整形板9により整形さ
れた流体負荷体である。12は前記電力計本体1
に設けられたレーザ光導入口であり、13は前記
レーザ光導入口12から導かれるレーザ光であ
る。14は校正用ヒータ、15は前記電力計本体
1の上部に設けられたブロワーである。
FIG. 1 is a three-dimensional perspective view showing the structure of a laser wattmeter which is an embodiment of the present invention. In the figure, reference numeral 1 denotes a cylindrical power meter main body, and the power meter main body 1 is provided with an introduction pipe 2 for introducing fluid H and a discharge pipe 3 for discharging the fluid H. 4 is a flow meter for measuring the flow rate of the fluid H, and is provided in the introduction pipe 2. 5 and 6 are temperature sensors for measuring the temperature of the fluid H; the temperature sensor 5 is provided in the introduction pipe 2 to measure the temperature before the laser beam is directed onto the fluid load; is provided in the discharge pipe 3 to measure the fluid velocity after irradiating the fluid load with a laser beam. 7 is a watering funnel for dropping the fluid H introduced into the power meter main body 1 in a shower style, 8 is a conical multilayer mesh, and 9 is the fluid H
This is a fluid load body shaping plate that guides the fluid to the irradiation position, and consists of a main body 9A shaped like a cap and a sub-body 9B similarly shaped like a cap provided at intervals above the main body 9A.The main body 9A has a hole in the upper center. A sub-body 9B is provided to cover this hole. Further, a gap 10 is partially formed between the main body 9A and the inner surface of the wattmeter main body 1, and the rest is sealed. 11 is a fluid load body shaped by the fluid load body shaping plate 9; 12 is the power meter main body 1
13 is a laser beam introduced from the laser beam introduction port 12. Reference numeral 14 represents a calibration heater, and reference numeral 15 represents a blower provided at the top of the power meter main body 1.

このブロワー15とじようろ7と多層メツシユ
8とで潜熱回収装置を構成する。
The blower 15, funnel 7, and multilayer mesh 8 constitute a latent heat recovery device.

次に、上記レーザ電力計の動作について説明す
る。電力計本体1内の気圧はブロワー15によつ
て常に大気圧より負圧に保たれ、蒸発した流体蒸
気がレーザ光導入口12から外に出ていかないよ
うにしてある。流体Hはポンプなどによつて導入
パイプ2に導かれ、流量計4を通つて落下する。
流量計4により流量が測定された流体Hは、温度
センサ5によりレーザ光13の照射前の温度が測
定され、前記潜熱回収装置に導かれ、流体負荷体
整形板9に達する。この流体負荷体整形板9はレ
ーザ光13を吸収するように流体Hをレーザ光導
入口12側には流れず反対側にのみ、すなわち照
射位置に導く。流体Hを流下させた状態で、測定
するレーザ光13をレーザ光導入口12から導入
すると、レーザ光13は流体Hに吸収され流体H
の温度が上昇すると共に流体Hの蒸気が発生す
る。この蒸気はブロワー15によつて吸引され、
流体負荷体整形板9の本体9Aの孔から副体9B
の下面側を通つて上昇し潜熱回収装置へと導かれ
る。潜熱回収装置へ導かれた蒸気はじようろ7よ
り細かい水滴状のシヤワーとなり、多層メツシユ
8により蒸気は再び液化し、流体Hの一部とな
る。この時、潜熱も流体Hに吸収され流体Hの温
度を上昇させる。そして流体Hは流体負荷体整形
板9を通り負荷体としてレーザ光13を吸収して
温度が上昇する。このようにして温度上昇した流
体Hは校正用ヒータ14を通つて温度センサ6に
より温度が測定される。
Next, the operation of the laser wattmeter will be explained. The air pressure inside the power meter main body 1 is always maintained at a negative pressure below the atmospheric pressure by the blower 15 to prevent the evaporated fluid vapor from going out through the laser light inlet 12. The fluid H is guided into the introduction pipe 2 by a pump or the like, and falls through the flow meter 4.
The temperature of the fluid H whose flow rate has been measured by the flowmeter 4 is measured by the temperature sensor 5 before being irradiated with the laser beam 13, and is led to the latent heat recovery device and reaches the fluid load body shaping plate 9. This fluid load body shaping plate 9 absorbs the laser beam 13 so that the fluid H does not flow toward the laser beam introduction port 12 but guides it only to the opposite side, that is, to the irradiation position. When the laser beam 13 to be measured is introduced from the laser beam introduction port 12 while the fluid H is flowing down, the laser beam 13 is absorbed by the fluid H.
As the temperature of the fluid H increases, vapor of the fluid H is generated. This steam is sucked by the blower 15,
From the hole in the main body 9A of the fluid load body shaping plate 9 to the secondary body 9B
It rises through the bottom side of the body and is led to the latent heat recovery device. The steam led to the latent heat recovery device becomes a shower of water droplets smaller than the water funnel 7, and the steam is liquefied again by the multilayer mesh 8 and becomes part of the fluid H. At this time, latent heat is also absorbed by the fluid H, increasing the temperature of the fluid H. Then, the fluid H passes through the fluid load body shaping plate 9 and absorbs the laser beam 13 as a load, thereby increasing its temperature. The temperature of the fluid H whose temperature has increased in this manner is measured by the temperature sensor 6 through the calibration heater 14.

上記のようにして得られた流体Hの流量と温度
変化から、次式によりレーザ光のレーザ電力Pが
測定できる。
From the flow rate and temperature change of the fluid H obtained as described above, the laser power P of the laser beam can be measured using the following equation.

P(KW)=4.18605÷60・A・ΔT・Q =0.0697・A・ΔT・Q ここで、 A:流体負荷体の吸収係数 ΔT:流体の温度上昇値〔℃〕 Q:流体の流量〔/min〕 たとえば、毎分1の流体が流れ、流体の温度
上昇が10℃とすると、レーザ電力は上式から
0.70AKWとなる。また、炭酸ガスレーザの場合
はレーザ光吸収負荷体として水を用いればよい
が、その他のレーザ光の場合は、色素を混入した
混合水を用いればレーザ電力が測定できる。
P (KW) = 4.18605÷60・A・ΔT・Q = 0.0697・A・ΔT・Q Where, A: Absorption coefficient ΔT of fluid load body: Temperature rise value of fluid [℃] Q: Fluid flow rate [/ min] For example, if the fluid flows at a rate of 1 per minute and the temperature rise of the fluid is 10°C, the laser power is calculated from the above equation.
It becomes 0.70AKW. Further, in the case of a carbon dioxide laser, water may be used as the laser light absorbing load, but in the case of other laser lights, the laser power can be measured by using mixed water containing a dye.

第2図は上記実施例によるレーザ電力計を用い
た炭酸ガスレーザ電力の測定と、レーザカロリー
メータ法によるレーザ電力の測定との比較データ
を示す図である。同図の実線は、レーザカロリー
メータ法と上記実施例による電力測定の関係を示
したものであり、点線はブロワー15とじようろ
7と多層メツシユ8により構成される潜熱回収装
置を停止した場合を示す。点線のごとく3KWか
らレーザ電力の測定は不可能となる。
FIG. 2 is a diagram showing comparison data between the measurement of carbon dioxide laser power using the laser power meter according to the above embodiment and the measurement of laser power using the laser calorimeter method. The solid line in the figure shows the relationship between the laser calorimeter method and the power measurement according to the above embodiment, and the dotted line shows the case when the latent heat recovery device composed of the blower 15, watering funnel 7, and multilayer mesh 8 is stopped. show. As shown by the dotted line, it becomes impossible to measure the laser power from 3KW.

第3図は、この発明によるレーザ電力計の過度
応答速度試験の結果を示す図である。同図aは立
下り特性を、同図bは立上り特性を示す。曲線A
が流体負荷測定法、曲線Bがレーザカロリーメー
タ法を示す。レーザカロリーメータ法では応答速
度が約20秒であつたが、流体負荷体による測定法
では4.5秒という非常に早い応答特性を得ること
ができる。大出力炭酸ガスレーザ電力の測定器で
このような早い過度応答特性を持つものは他に例
がない。
FIG. 3 is a diagram showing the results of a transient response speed test of the laser power meter according to the present invention. Figure a shows the falling characteristic, and Figure b shows the rising characteristic. Curve A
curve B shows the fluid load measurement method and curve B shows the laser calorimeter method. In the laser calorimeter method, the response time was approximately 20 seconds, but in the measurement method using a fluid load, an extremely fast response characteristic of 4.5 seconds can be obtained. There is no other high-output carbon dioxide laser power measuring instrument with such fast transient response characteristics.

なお、上記実施例では流量計4を電力計本体1
の上部導入パイプ2に設けたが、流量計4は流量
を測定するためのものであるから設置場所は導入
パイプ2以外の場所でもよいことは当然である。
また、流体Hは水以外のものであつてもよい。
In addition, in the above embodiment, the flow meter 4 is connected to the power meter main body 1.
However, since the flowmeter 4 is for measuring flow rate, it is natural that it may be installed at a location other than the introduction pipe 2.
Further, the fluid H may be something other than water.

以上説明したように、この発明に係るレーザ電
力測定方法は、流体がレーザ光を吸収するという
性質を利用し、流体にレーザ光を照射すると共
に、その照射によつて発生する流体蒸気の潜熱を
流体に回収し、レーザ光照射前の流体温度と照射
後の流体温度および流体の流量からレーザ光の電
力を測定するようにしたので、各種レーザのレー
ザ電力を簡単に測定できる。特に大電力のレーザ
光の測定が可能である極めて優れた効果を有す
る。
As explained above, the laser power measurement method according to the present invention takes advantage of the property that fluid absorbs laser light, irradiates the fluid with laser light, and calculates the latent heat of the fluid vapor generated by the irradiation. Since the power of the laser light is measured from the fluid temperature before laser light irradiation, the fluid temperature after irradiation, and the flow rate of the fluid, the laser power of various lasers can be easily measured. In particular, it has an extremely excellent effect in that it is possible to measure high-power laser light.

【図面の簡単な説明】[Brief explanation of drawings]

第1図はこの発明の一実施例をなすレーザ電力
計の構造を示す立体透視図、第2図は第1図に示
すレーザ電力計による測定結果とレーザカロリー
メータ法による測定結果を比較したデータを示す
図、第3図は第1図に示すレーザ電力計の過渡応
答速度を示す図である。 図中、1は電力計本体、2は導入パイプ、3は
排出パイプ、4は流量計、5,6は温度センサ、
7はじようろ。8は多層メツシユ、9は流体負荷
体整形板、10は間隙、11は流体負荷体、12
はレーザ光導入口、13はレーザ光、14は校正
用ヒータ、15はブロワーである。
Fig. 1 is a three-dimensional perspective view showing the structure of a laser wattmeter that is an embodiment of the present invention, and Fig. 2 is data comparing the measurement results by the laser wattmeter shown in Fig. 1 and the measurement results by the laser calorimeter method. FIG. 3 is a diagram showing the transient response speed of the laser power meter shown in FIG. 1. In the figure, 1 is the power meter body, 2 is the introduction pipe, 3 is the discharge pipe, 4 is the flow meter, 5 and 6 are the temperature sensors,
7 is the playground. 8 is a multilayer mesh, 9 is a fluid load body shaping plate, 10 is a gap, 11 is a fluid load body, 12
13 is a laser beam introduction port, 13 is a laser beam, 14 is a calibration heater, and 15 is a blower.

Claims (1)

【特許請求の範囲】[Claims] 1 レーザ光吸収負荷体として液体を用い、この
流体にレーザ光を照射すると共に、レーザ光照射
により発生する流体蒸気の潜熱を潜熱回収装置で
前記流体に回収し、前記レーザ光照射前の流体温
度と照射後の液体温度および前記流体の流量とか
ら、レーザ光の電力を測定することを特徴とする
レーザ電力測定方法。
1 Using a liquid as a laser beam absorption load, irradiating this fluid with a laser beam, and recovering the latent heat of the fluid vapor generated by the laser beam irradiation into the fluid using a latent heat recovery device, to reduce the temperature of the fluid before the laser beam irradiation. A method for measuring laser power, comprising: measuring the power of a laser beam from the temperature of the liquid after irradiation and the flow rate of the fluid.
JP5218383A 1983-03-28 1983-03-28 Measuring method of laser electric power Granted JPS59176631A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5218383A JPS59176631A (en) 1983-03-28 1983-03-28 Measuring method of laser electric power

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5218383A JPS59176631A (en) 1983-03-28 1983-03-28 Measuring method of laser electric power

Publications (2)

Publication Number Publication Date
JPS59176631A JPS59176631A (en) 1984-10-06
JPH025250B2 true JPH025250B2 (en) 1990-02-01

Family

ID=12907686

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5218383A Granted JPS59176631A (en) 1983-03-28 1983-03-28 Measuring method of laser electric power

Country Status (1)

Country Link
JP (1) JPS59176631A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR101121057B1 (en) 2009-06-26 2012-03-16 한국기초과학지원연구원 Calorimetric measurement system of the microwave output power

Also Published As

Publication number Publication date
JPS59176631A (en) 1984-10-06

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